For me the fourier transform of a measure $\mu\in\mathcal{S}'(\mathbb{R})$ is defined by $\hat{\mu}(\varphi)=\mu(\hat{\varphi})$ where $\varphi\in\mathcal{S}(\mathbb{R})$.
My question is: if one has $\int_\mathbb{R}\operatorname{e}^{-\lambda s}d\mu(s)=f(\lambda)$ for all $\Re(\lambda)>0$, and if $f$ has a continuous prolonging on $\Re(z)=0$ with $t\mapsto f(t)\in \operatorname{L}^1_{loc}(\mathbb{R})$, can we conclude that the Fourier transform of $\mu$ is $t\mapsto f(2i\pi t)$?
My question comes from arithmetic context: with $\mu=\sum_{p\in\mathbb{P}}\frac{1}{p}\delta_{\log{p}}$ we have easely that $\int_\mathbb{R}e^{-\lambda t}d\mu(t)=\zeta_\mathbb{P}(1+\lambda)$ and I'd like to conclude that $\hat{\mu}=\zeta_{\mathbb{P}}(1+2i\pi t)$. I know a specific proof of that but I'd like to know if it were a general thing.